S.J. Jones* and H.K.D.H. Bhadeshia,
Phase Transformations Group,
Department of Materials Science and Metallurgy,
University of Cambridge,
Cambridge, U.K.
*Dr S.J. Jones is now with Ford Motor Co. (UK) Ltd.
To calculate the heterogeneous activation energy barrier to nucleation on a spherical substrate such as an inclusion using classical nucleation theory.
Language: | FORTRAN |
Product form: | Source code |
SUBROUTINE MAP_INC_POTENCY(INCGMAX1VOL,GMAX1VOL, & RI,UFAFENERGY,FAFENERGY,FIENERGY,AIENERGY,AEB, & AEBHOMOG,FRACHOMAEB) DOUBLE PRECISION INCGMAX1VOL,GMAX1VOL,RI,UFAFENERGY, & FAFENERGY,FIENERGY,AIENERGY,AEB,AEBHOMOG,FRACHOMAEB DOUBLE PRECISION PI,RC,TESTIT,PHI,SEPN,PSI,THETA,BETA, & FUNCTHETA,FUNCPSI,FUNCBETA,VS,VC1,VC2,VC3,XHGT,YHGT,AS, & AC1,AC2,AC4,AF
PARAMETER (PI=3.141592654)
Barritte [2] developed a model for the activation energy barrier to nucleation on a spherical substrate by assuming that the 'wetting' angle is fixed at 90°. This new model removes this assumption.
Name | Type | Description |
---|---|---|
INCGMAX1VOL | real | maximum possible thermodynamic driving force for nucleation local to the spherical substrate, per unit volume (Jm-3). |
GMAX1VOL | real | maximum possible thermodynamic driving force for nucleation remote from the spherical substrate, per unit volume (Jm-3). |
RI | real | radius of the spherical substrate(m). |
UFAFENERGY | real | interfacial energy per unit area at a disordered boundary between the product and the parent phases (Jm-2 ). |
FAFENERGY | real | interfacial energy per unit area at a facetted (coherent) boundary between the product and the parent phases (Jm-2 ). |
FIENERGY | real | interfacial energy per unit area between the product phase and the spherical substrate (Jm-2 ). |
AIENERGY | real | interfacial energy per unit area between the parent phase and the spherical substrate (Jm-2 ). |
Name | Type | Description |
---|---|---|
AEB | real | activation energy barrier to nucleation at the spherical substrate (J). |
AEBHOMOG | real | activation energy barrier to homogeneous nucleation remote from the spherical substrate (J). |
FRACHOMAEB | real | ratio between AEB and AEBHOMOG. This is the effective 'shape' factor for nucleation on the spherical substrate. |
No information supplied.
None.
DOUBLE PRECISION GMAX1VOL,RI,UFAFENERGY,FAFENERGY, & FIENERGY,AIENERGY,AEB,AEBHOMOG,FRACHOMAEB,INCGMAX1VOL READ(*,*) INCGMAX1VOL,GMAX1VOL,RI,UFAFENERGY,FAFENERGY, & FIENERGY,AIENERGY C CALL MAP_STEEL_INC_POTENCY(INCGMAX1VOL,GMAX1VOL,RI,UFAFENERGY, & FAFENERGY,FIENERGY,AIENERGY,AEB,AEBHOMOG,FRACHOMAEB) C WRITE(*,10) AEB,AEBHOMOG,FRACHOMAEB 10 FORMAT(E10.3,1X,E10.3,1X,E10.3) STOP END
-0.260E7 -0.260E7 0.270E-6 0.500E-1 0.363E-1 0.463E-1 0.623E-1
0.814E-16 0.310E-15 0.263E0
None.
activation, energy, barrier, nucleation, classical, spherical, substrate, inclusion, heterogeneous, homogeneous
MAP originated from a joint project of the National Physical Laboratory and the University of Cambridge.
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